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ECE 340 Lecture 41 : MOSFET II

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ECE 340 Lecture 41 : MOSFET II ECE 340 Lecture 41 : MOSFET II Class Outline: •Mobility Models •Short Channel Effects •Logic Devices Things you should know when you leave… Key Questions • Why is the mobility in the channel lower than in the bulk? • Why do strong electric fields degrade channel mobility ? • What is the major difference between long channel and short channel MOSFETs? • How can I turn these into useful logic devices? M.J. Gilbert ECE 340 – Lecture 41 12/10/12 MOSFET Output Characteristics This makes sense based on what we already know about MOSFETs… For low drain voltages, the MOSFET looks like a resistor if the MOSFET is above threshold and depending on the value of VG. Now we can obtain the conductance of the channel… +++++++++++++ ++++ - - - - - - •But again, this is only valid in the linear regime. •We are assuming that VD << VG – VT. Depletion Region Channel Region M.J. Gilbert ECE 340 – Lecture 41 12/10/12 MOSFET Output Characteristics So we can describe the linear +++++++++++++ ++++ Pinch off regime, but how do we describe the VD saturation regime… - - - - - - • As the drain voltage is increased, the voltage across the oxide decreases near the drain end. • The resulting mobile charge also decreases in the channel Depletion Region Channel Region near the drain end. • To obtain an expression for the drain current in saturation, substitute in the saturation condition. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 MOSFET Output Characteristics Let’s summarize the output characteristics for NMOS and PMOS… - - - - - - NMOS P-type Si + + + + + + + + + + + + + PMOS N-type Si M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models Let’s try a simple problem… For an n-channel MOSFET with a gate oxide thickness of 10 nm, VT = 0.6 V and Z =25 µm and a channel length of 1 µm. Calculate the drain current at VG = 5V and VD = 0.1 V. Repeat the process for VG = 3 V and VD = 5 V. Discuss what happens for VD = 7 V. Assume an electron channel mobility of 200 cm2/V*sec. −14 εi (3.9)8.85×10 −7 F Let’s start by finding the insulator capacitance… C = = ( ) = 3.45×10 i d 10 −6 cm 2 For the first set of given parameters VD < (VG-VT) so we are in the linear regime… Z ⎡ 1 2 ⎤ I D = µnCi (VG −VT )VD − VD L ⎣⎢ 2 ⎦⎥ −4 I D = 7.51×10 A For the second set of given parameters… VD = 5 V and (VG - VT) = 2.4 V 2 Z ⎡ sat 1 sat ⎤ Nothing happens for VD I D = µnCi (VG −VT )VD − (VD ) We are in saturation… L ⎣⎢ 2 ⎦⎥ = 7 V as we are well into the non-linear I 4.97 10 −3 A D = × regime. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models But all of these models depend on the effective carrier mobility… Remember the mobility? I Ex We want to define a current, or charge per unit time crossing of observation orientated normal to the direction of current flow. drift J n = −qn vdn = qnµn E drift J p = qp vdp = qpµ p E Proportional to: •Carrier drift velocity •Carrier concentration •Carrier charge M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models And from the definition of the current, we can define the mobility… drift Using the definitions for the hole and electron J n = −qn vdn = qnµn E drift currents: drift J p = qp vdp = qpµ p E The electron and hole mobility then becomes: qτ c µn = * Electron Mobility 2mn What can we say about the qτ mobility in general? µ = c p 2m* Hole Mobility p •Refers to the ease with which carriers move through a host crystal. In units of: M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models What does temperature mean to mobility? Silicon mobility at 300 K Lattice Scattering Ionized Impurity Scattering M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models Seems like there are two main competing phenomena… Impurity (dopant) Scattering: •The force acting on the particles is Coulombic. •There is less change in the - + electron’s direction of travel 3 the faster it goes. 3 2 vth T µimpurity ∝ ∝ N A + N D N A + N D Phonon (lattice) Scattering: 3 q − τ phonon 1 1 2 µ phonon = * ∝ ∝ 1/ 2 ∝ T m # phonons ×vth T ×T Phonon scattering mobility decreases as the temperature increases. Since the scattering probability is inversely proportional 1 1 to the mean free time and the mobility, we can add = individual scattering mechanisms inversely. µ µ phonon + µimpurity M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models We know bulk mobility, what makes the channel mobility different? There are now more scattering mechanisms and the electrons are confined to a smaller space in the channel… VG Source Drain - - - - - - - - - - - - - We have additional - - - - - - VD surface roughness - - - - scattering… SiO2 Si M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models What does the surface actually look like? Gate - E F •Electric field needed to invert Parameters Mean ∆ VT/ Mean ∆SS / Mean ∆(Ion/Ioff) V V SS SS I /I surface pulls electrons closer to T T on off /(Ion/Ioff) the gate interface. •More field increases the Units (mV) % (mV/ % % interaction with the surface. decade •This leads to a decrease in ) mobility not seen in the bulk. No SR . 93.11 10.23 68.08 3.49 692 15.46 Fixed SR . 127.5 14.9 70.33 3.45 741 19.56 M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models We are also aware of the fact that there can be stray charges present in the insulating oxide… • Alkali metals can easily be incorporated in the oxide during the fabrication process. • These metals induce positive charges in the oxides which induce negative charges in the semiconductor. • The magnitude of the effect depends on the number of sodium atoms and their distance from the surface. • The atoms may drift in applied fields which leads to a continuous change in the threshold voltage. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models What about oxide charges? • Positive charges arise from interface states at the Si-SiO2 interface. • When oxidation is stopped, some ionic silicon is left near the surface. • These ions along with other uncoupled bonds forms a sheet of positive charge at the interface. • The charges depend Why are devices made on [100] instead of [111]? on oxidation rate, heat treatment, and •Because interface charges are 10x higher on crystal orientation. [111] relative to [100]. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models So how do they effect the effective mobility? VG Source + + + + Drain - - - - - - - - - - - - VD - - - - •Coulomb interactions between the electrons in the channel and the trapped oxide charges present another scattering rate not seen in the bulk. •If we plot the effective carrier mobility in a MOSFET as a function of the average transverse electric field we get the universal mobility degredation curve. •The curve is valid for any MOSFET independent of device and structural parameters such as oxide thickness. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models So how do we determine the transverse electric field? We determine the transverse field by applying Gauss’ Law… Q D dS dv = ∫ ⋅ = ∫ ρv S v From this we can find the average transverse field in the middle of the channel… We can often express the degradation by rewriting the drain current equation… New term causes drain current to increase sub- linearly with gate bias for Mobility degradation large biases. parameter M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Mobility Models But there is also a strong dependence of the longitudinal electric field… •Carrier drift velocity increases linearly with electric field until it saturates. •After saturation, mobility no longer makes any sense. px qτ c Ex vx = * = ± * Let’s describe the velocity in the following way… mn, p mn, p The maximum longitudinal field is the voltage drop near the drain end divided by the length of the pinch-off region. where ΔL ≈ 2tOX x j M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Short Channel Effects Analyzing must be modified in short channel devices… •Effective channel mobility decreases with increasing transverse perpendicular electric field to the gate oxide. •For very high longitudinal electric fields in the pinch-off region, the carrier velocity saturates. •In a short channel device, the carriers travel at the saturation velocity for most of the channel. •Drain current does not increase quadratically with VG – VT but now has a linear dependence. M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Logic Devices We know a lot about MOSFETs, now we seek to understand their use in digital logic, the simplest of which is the inverter… One of the most important concepts in inverters is the voltage transfer characteristic. There are 5 key points in the voltage transfer characteristic… I. Logic high or “1” (VOH) II. Logic low or “0” (VOL) Unity gain points are useful because if III. Intersection of line with unity slope the input voltage in in between them, (VOUT = VIN). then the output signal is amplified. IV. Unity gain point VIL Important for noise considerations too. V. Unity gain point VIH M.J. Gilbert ECE 340 – Lecture 41 12/10/12 Logic Devices So how do we determine the voltage transfer characteristic (VTC)? •Consider the simple inverter circuit shown to the right… •In the output loop of the circuit, we see that from the power supply to ground, the current through the resistor is the same as ID.
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